
To address this problem, we will examine the thermodynamical processes depicted in the figure and the given options, focusing on the relationships between molar heat capacities. The relevant molar heat capacities are \( C_A \), \( C_B \), \( C_P \), and \( C_V \).
The figure illustrates two primary processes, designated as \( A \) and \( B \). Let's analyze each individually:
The option that aligns with our analysis is:
\( C_A = 0 \, \text{and} \, C_B = \infty \)
This conclusion is supported by the analysis of the thermodynamical processes and their graphical representation on the log-log diagram.
A real gas within a closed chamber at \( 27^\circ \text{C} \) undergoes the cyclic process as shown in the figure. The gas obeys the equation \( PV^3 = RT \) for the path A to B. The net work done in the complete cycle is (assuming \( R = 8 \, \text{J/molK} \)):
